4.5 Article

Doubly-heavy tetraquark states cc(u)over-bar(d)over-bar and bb(u)over-bar(d)over-bar

期刊

CHINESE PHYSICS C
卷 46, 期 5, 页码 -

出版社

IOP Publishing Ltd
DOI: 10.1088/1674-1137/ac4ee8

关键词

tetraquarks; quark model; real scaling method

资金

  1. National Natural Science Foundation of China [11847145, 11865019]

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This study explores bound states and low-lying resonance states of doubly-heavy tetraquark states cc (u) over bar(d) over bar (T-cc) and bb (u) over bar(d) over bar (T-bb) using a chiral quark model and accurate few-body method, Gaussian expansion method. The results reveal important findings regarding the binding energy and resonance states of these systems.
Inspired by the recent observation of a very narrow state, called T-cc(+),by the LHCb collaboration, the possible bound states and low-lying resonance states of the doubly-heavy tetraquark states cc (u) over bar(d) over bar (T-cc) and bb (u) over bar(d) over bar (T-bb) are searched in the framework of a chiral quark model with an accurate few-body method, the Gaussian expansion method. The real scaling method is also applied to identify the genuine resonance states. In the calculation, the meson-meson structure, diquark-antidiquark structure, and their coupling are all considered. The numerical results show: (i) For T-cc and T-bb, only I(J(P)) = 0(1(+)) states are bound in different quark structures. The binding energy varies from a few MeV for the meson-meson structure to over 100 MeV for the diquark-antidiquark structure. For example, for T-cc in the meson-meson structure, there exists a weakly bound molecule DD* state around 3841.4 MeV, 1.8 MeV below the (DD)-D-0*(+) , which may be a good candidate for the observed state by LHCb; however in the diquark-antidiquark structure, a deeper bound state with mass 3700.9 MeV is obtained. When considering the structure mixing, the energy of system decreases to 3660.7 MeV and the shallow bound state disappears. (ii) Besides bound states, several resonance states for T-QQ(Q = c, b) with I(J(P)) = 1(0(+)), 1(1(+)), 1(2(+)), 0(1(+)) are proposed.

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